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Observation and enhancement of room temperature bilinear magnetoelectric resistance in sputtered topological semimetal Pt3Sn 观察并增强溅射拓扑半金属 Pt3Sn 的室温双线性磁电电阻
Pub Date : 2024-07-17 DOI: 10.1038/s44306-024-00036-1
Yihong Fan, Zach Cresswell, Yifei Yang, Wei Jiang, Yang Lv, Thomas J. Peterson, Delin Zhang, Jinming Liu, Tony Low, Jian-Ping Wang
Topological semimetal materials have attracted a great deal of attention due to their intrinsic strong spin-orbit coupling, which leads to large charge-to-spin conversion efficiency and novel spin transport behaviors. In this work, we have observed a bilinear magnetoelectric resistance (BMER) of up to 0.0034 nm2A−1Oe−1 in a single layer of sputtered semimetal Pt3Sn at room temperature. Being different from previous works, the value of BMER in sputtered Pt3Sn does not change out-of-plane due to the polycrystalline nature of the Pt3Sn layer. The observation of BMER provides strong evidence of the existence of spin-momentum locking in the sputtered polycrystalline Pt3Sn. By adding an adjacent CoFeB magnetic layer, the BMER value of this bilayer system is doubled compared to the single Pt3Sn layer. This work broadens the material system in BMER study, which paves the way for the characterization of topological states and applications for spin memory and logic devices.
拓扑半金属材料因其固有的强自旋轨道耦合而备受关注,这种耦合可带来巨大的电荷-自旋转换效率和新颖的自旋传输行为。在这项工作中,我们观察到室温下单层溅射半金属 Pt3Sn 的双线性磁电电阻(BMER)高达 0.0034 nm2A-1Oe-1。与之前的研究不同的是,由于 Pt3Sn 层的多晶性质,溅射 Pt3Sn 的 BMER 值在平面外没有变化。对 BMER 的观测为溅射多晶铂锰中存在自旋动量锁定提供了有力证据。通过添加相邻的 CoFeB 磁层,该双层系统的 BMER 值比单层 Pt3Sn 增加了一倍。这项工作拓宽了 BMER 研究的材料体系,为拓扑状态的表征以及自旋存储器和逻辑器件的应用铺平了道路。
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引用次数: 0
Wideband coherent microwave conversion via magnon nonlinearity in a hybrid quantum system 通过混合量子系统中的磁子非线性实现宽带相干微波转换
Pub Date : 2024-07-02 DOI: 10.1038/s44306-024-00035-2
Jiahao Wu, Jiacheng Liu, Zheyu Ren, Man Yin Leung, Wai Kuen Leung, Kin On Ho, Xiangrong Wang, Qiming Shao, Sen Yang
Frequency conversion is a widely realized physical process in nonlinear systems of optics and electronics. As an emerging nonlinear platform, spintronic devices have the potential to achieve stronger frequency conversion. Here, we demonstrated a microwave frequency conversion method in a hybrid quantum system, integrating nitrogen-vacancy centers in diamond with magnetic thin film CoFeB. We achieve a conversion bandwidth ranging from 0.1 to 12 GHz, presenting an up to 25th order frequency conversion and further display the application of this method for frequency detection and qubits coherent control. Distinct from traditional frequency conversion techniques based on nonlinear electric response, our approach employs nonlinear magnetic response in spintronic devices. The nonlinearity, originating from the symmetry breaking such as domain walls in magnetic films, presents that our method can be adapted to hybrid systems of other spintronic devices and spin qubits, expanding the application scope of spintronic devices and providing a promising on-chip platform for coupling quantum systems.
频率转换是光学和电子学非线性系统中广泛实现的物理过程。作为一种新兴的非线性平台,自旋电子器件具有实现更强频率转换的潜力。在这里,我们展示了一种混合量子系统中的微波频率转换方法,它将金刚石中的氮空位中心与磁性薄膜 CoFeB 集成在一起。我们实现了 0.1 至 12 GHz 的转换带宽,呈现了高达 25 阶的频率转换,并进一步展示了这种方法在频率检测和量子比特相干控制方面的应用。与基于非线性电响应的传统频率转换技术不同,我们的方法采用了自旋电子器件中的非线性磁响应。这种非线性源于磁性薄膜中的畴壁等对称性破缺,表明我们的方法可适用于其他自旋电子器件和自旋量子比特的混合系统,从而扩大了自旋电子器件的应用范围,并为耦合量子系统提供了一个前景广阔的片上平台。
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引用次数: 0
Magnetic anisotropy and GGG substrate stray field in YIG films down to millikelvin temperatures 温度低至毫开尔文的 YIG 薄膜中的磁各向异性和 GGG 基底杂散磁场。
Pub Date : 2024-07-02 DOI: 10.1038/s44306-024-00030-7
Rostyslav O. Serha, Andrey A. Voronov, David Schmoll, Roman Verba, Khrystyna O. Levchenko, Sabri Koraltan, Kristýna Davídková, Barbora Budinská, Qi Wang, Oleksandr V. Dobrovolskiy, Michal Urbánek, Morris Lindner, Timmy Reimann, Carsten Dubs, Carlos Gonzalez-Ballestero, Claas Abert, Dieter Suess, Dmytro A. Bozhko, Sebastian Knauer, Andrii V. Chumak
Quantum magnonics investigates the quantum-mechanical properties of magnons, such as quantum coherence or entanglement for solid-state quantum information technologies at the nanoscale. The most promising material for quantum magnonics is the ferrimagnetic yttrium iron garnet (YIG), which hosts magnons with the longest lifetimes. YIG films of the highest quality are grown on a paramagnetic gadolinium gallium garnet (GGG) substrate. The literature has reported that ferromagnetic resonance (FMR) frequencies of YIG/GGG decrease at temperatures below 50 K despite the increase in YIG magnetization. We investigated a 97 nm-thick YIG film grown on 500 μm-thick GGG substrate through a series of experiments conducted at temperatures as low as 30 mK, and using both analytical and numerical methods. Our findings suggest that the primary factor contributing to the FMR frequency shift is the stray magnetic field created by the partially magnetized GGG substrate. This stray field is antiparallel to the applied external field and is highly inhomogeneous, reaching up to 40 mT in the center of the sample. At temperatures below 500 mK, the GGG field exhibits a saturation that cannot be described by the standard Brillouin function for a paramagnet. Including the calculated GGG field in the analysis of the FMR frequency versus temperature dependence allowed the determination of the cubic and uniaxial anisotropies. We find that the total crystallographic anisotropy increases more than three times with the decrease in temperature down to 2 K. Our findings enable accurate predictions of the YIG/GGG magnetic systems behavior at low and ultralow millikelvin temperatures, crucial for developing quantum magnonic devices.
量子磁学研究磁子的量子力学特性,如量子相干性或纠缠,用于纳米尺度的固态量子信息技术。量子磁子学最有前途的材料是铁磁性钇铁石榴石(YIG),它所承载的磁子寿命最长。最高质量的 YIG 薄膜是在顺磁性钆镓石榴石(GGG)基底上生长的。据文献报道,尽管 YIG 的磁化率增加,但在温度低于 50 K 时,YIG/GGG 的铁磁共振 (FMR) 频率会降低。我们使用分析和数值方法,在低至 30 mK 的温度下进行了一系列实验,研究了生长在 500 μm 厚 GGG 衬底上的 97 nm 厚 YIG 薄膜。我们的研究结果表明,导致 FMR 频率偏移的主要因素是部分磁化的 GGG 衬底产生的杂散磁场。这种杂散磁场与外加磁场反平行,而且高度不均匀,在样品中心可达 40 mT。在低于 500 mK 的温度下,GGG 场呈现饱和状态,无法用准磁体的标准布里渊函数来描述。将计算出的 GGG 场纳入 FMR 频率随温度变化的分析中,可以确定立方各向异性和单轴各向异性。我们发现,随着温度降低到 2 K,总晶体学各向异性增加了三倍多。我们的研究结果能够准确预测 YIG/GGG 磁性系统在低温和超低毫开尔文温度下的行为,这对开发量子磁性器件至关重要。
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引用次数: 0
Antiferromagnetic spintronics and beyond 反铁磁自旋电子学及其他
Pub Date : 2024-07-02 DOI: 10.1038/s44306-024-00029-0
A. Dal Din, O. J. Amin, P. Wadley, K. W. Edmonds
In this review article, we summarize some recent key results in the development of antiferromagnetic spintronics. Current-induced switching of the Néel vector orientation has now been established in a wide range of antiferromagnetic films and antiferromagnet / heavy metal bilayers, as well as current-driven motion of antiferromagnetic spin textures. The latter are particularly promising due to their small size and topological stability, but reading their magnetic state presents challenges. We also focus on materials whose compensated spin arrangements (either collinear or noncollinear) are coexistent with a spin-split band structure, enabling first-order spintronic phenomena including giant and tunneling magnetoresistance, and the anomalous Hall effect. The resulting combination of efficient electrical readout mechanisms with the advantages of a near-zero net magnetization has potential to be transformative for spintronic applications.
在这篇综述文章中,我们总结了反铁磁自旋电子学发展的一些最新关键成果。目前已在多种反铁磁薄膜和反铁磁/重金属双层膜中实现了电流诱导的奈尔矢量方向转换,以及电流驱动的反铁磁自旋纹理运动。后者因其尺寸小和拓扑稳定性而特别有前景,但读取其磁性状态却面临挑战。我们还重点研究了补偿自旋排列(共线性或非共线性)与自旋分裂带结构共存的材料,从而实现了一阶自旋电子现象,包括巨磁电阻、隧道磁阻和反常霍尔效应。由此产生的高效电子读出机制与近零净磁化的优势相结合,有望为自旋电子应用带来变革。
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引用次数: 0
Sub-millimeter propagation of antiferromagnetic magnons via magnon-photon coupling 通过磁子-光子耦合实现反铁磁磁子的亚毫米级传播
Pub Date : 2024-07-02 DOI: 10.1038/s44306-024-00034-3
Ryo Kainuma, Keita Matsumoto, Toshimitsu Ito, Takuya Satoh
For the realization of magnon-based current-free technologies, referred to as magnonics, all-optical control of magnons is an important technique for both fundamental research and practical applications. Magnon-polariton is a coupled state of magnon and photon in a magnetic medium, expected to exhibit magnon-like controllability and photon-like high-speed propagation. While recent studies have observed magnon-polaritons as modulation of incident terahertz waves, the influence of magnon-photon coupling on magnon propagation properties remains unexplored. This study aimed to observe the spatiotemporal dynamics of coherent magnon-polaritons through time-resolved imaging measurements. BiFeO3 was selected as the sample due to its anticipated strong coupling between magnons and photons. The observed dynamics suggest that antiferromagnetic magnons can propagate over long distances, up to hundreds of micrometers, through strong coupling with photons. These results enhance our understanding of the optical control of magnonic systems, thereby paving the way for terahertz opto-magnonics.
为了实现基于磁子的无电流技术(简称磁子学),磁子的全光控制是基础研究和实际应用的一项重要技术。磁子-极化子是磁介质中磁子和光子的耦合态,有望表现出类似磁子的可控性和类似光子的高速传播性。虽然最近的研究已经观察到磁子-极化子对入射太赫兹波的调制作用,但磁子-光子耦合对磁子传播特性的影响仍有待探索。本研究旨在通过时间分辨成像测量来观察相干磁子-极化子的时空动态。之所以选择 BiFeO3 作为样品,是因为预计磁子与光子之间会产生强耦合。观察到的动态表明,反铁磁性磁子可以通过与光子的强耦合进行长距离传播,最远可达数百微米。这些结果加深了我们对磁子系统光学控制的理解,从而为太赫兹光磁学铺平了道路。
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引用次数: 0
Spintronic devices for biomedical applications 用于生物医学应用的自旋电子器件
Pub Date : 2024-07-02 DOI: 10.1038/s44306-024-00031-6
Shahriar Mostufa, Shuang Liang, Vinit Kumar Chugh, Jian-Ping Wang, Kai Wu
In the past decade, there has been a significant rise in the development of novel spintronic device architectures specifically designed to meet the demands of diverse biomedical applications. These advancements have notably focused on enhancing various bioassay detection techniques, including magnetocardiography and neural signal recording. Through collaboration within the spintronics community, these devices are rapidly transitioning from laboratory prototypes to practical applications, catering to diverse biomedical applications and benefiting both researchers and medical practitioners alike. In this review, we comprehensively explore the biomedical applications of spintronic devices, due to their inherent sensitivity to external magnetic fields, ease of fabrication into large arrays of nano/micro-sized devices within confined spaces, resilience under harsh environmental conditions, and high repeatability. Established spintronics devices that exploit various magnetoresistive effects have already been extensively deployed as magnetic biosensors for disease diagnosis, medical imaging, and bio-magnetic field detection, offering superior sensitivity and robustness. This review aims to provide peers with an up-to-date overview of spintronic devices in biomedical contexts while also commenting on future research trends and challenges. With advancements in nano/microfabrication techniques enhancing device robustness and magnetic field sensitivity, it is foreseeable that these spintronic devices could catalyze revolutionary transformations in healthcare.
在过去十年中,为满足各种生物医学应用需求而专门设计的新型自旋电子器件架构的开发有了显著的增长。这些进步主要集中在增强各种生物检测技术上,包括磁心动图和神经信号记录。通过自旋电子学界的合作,这些设备正迅速从实验室原型过渡到实际应用,满足了各种生物医学应用的需求,使研究人员和医疗从业人员都受益匪浅。在这篇综述中,我们将全面探讨自旋电子器件的生物医学应用,因为它们对外部磁场具有固有的敏感性,易于在有限的空间内制造成大型纳米/微米级器件阵列,在恶劣的环境条件下具有很强的适应能力,并且具有很高的可重复性。利用各种磁阻效应的成熟自旋电子器件已被广泛应用于疾病诊断、医学成像和生物磁场检测的磁性生物传感器,具有卓越的灵敏度和稳健性。本综述旨在为同行提供生物医学领域自旋电子器件的最新概况,同时对未来的研究趋势和挑战进行评论。随着纳米/微细加工技术的进步,这些自旋电子器件的坚固性和磁场灵敏度都得到了提高,可以预见,它们将推动医疗保健领域的革命性变革。
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引用次数: 0
Emergence of exchange bias in van der Waals magnetic alloy CrxPt1−xTe2 范德华磁性合金 CrxPt1-xTe2 中交换偏压的出现
Pub Date : 2024-07-02 DOI: 10.1038/s44306-024-00028-1
Ryan Bailey-Crandell, Warren L. B. Huey, Archibald J. Williams, Wenyi Zhou, Joshua E. Goldberger, Roland K. Kawakami
CrxPt1−xTe2 is a recently developed van der Waals magnetic alloy noted for its stability under ambient conditions. Here, we report the emergence of an exchange bias effect in CrxPt1−xTe2, without typical exchange bias sources such as an adjacent antiferromagnetic layer. We find that the exchange bias is present for x = 0.45 and absent for x = 0.35, which is correlated to the presence of a Cr modulation where the Cr concentration alternates each vdW layer (modulation period of 2 layers) for x ≥ 0.4. We perform Monte Carlo simulations utilizing exchange parameters from first-principles calculations, which recreate the exchange bias in hysteresis loops of Cr0.45Pt0.55Te2. From our simulations, we infer the source of exchange bias to be magnetic moments locked into free energy minima that resist magnetization reversal. This work presents a way to introduce desirable magnetic properties to van der Waals magnets.
CrxPt1-xTe2 是最近开发的范德华磁性合金,因其在环境条件下的稳定性而备受关注。在这里,我们报告了在 CrxPt1-xTe2 中出现的交换偏压效应,而没有典型的交换偏压源,如相邻的反铁磁层。我们发现在 x = 0.45 时存在交换偏压,而在 x = 0.35 时则不存在交换偏压,这与存在铬调制有关,在 x ≥ 0.4 时,铬浓度会交替出现在每个 vdW 层(调制周期为 2 层)。我们利用第一原理计算得出的交换参数进行蒙特卡罗模拟,再现了 Cr0.45Pt0.55Te2 磁滞环中的交换偏置。根据模拟结果,我们推断交换偏压的来源是被锁定在自由能最小值的磁矩,这些磁矩会抵制磁化反转。这项研究提出了一种为范德华磁体引入理想磁性的方法。
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引用次数: 0
Spintronics meets orbitronics: Emergence of orbital angular momentum in solids 自旋电子学与轨道电子学的结合:固体中轨道角动量的出现
Pub Date : 2024-06-28 DOI: 10.1038/s44306-024-00023-6
Daegeun Jo, Dongwook Go, Gyung-Min Choi, Hyun-Woo Lee
One of the ultimate goals of spintronics is to realize an efficient electrical manipulation of spin for high-speed and low-power nanodevices. A core ingredient for achieving this goal is the relativistic interaction between the electron’s orbital motion and spin, but the properties of the orbital angular momentum itself have remained largely unexplored. However, recent theories and experiments have uncovered that electrons may acquire nonvanishing orbital angular momentum when an external electric field is applied, even without the spin–orbit coupling. These findings have spurred the emergence of a burgeoning field known as orbitronics, which harnesses the orbital angular momentum to manipulate magnetic devices. In this Review, we provide an overview of the recent developments in orbitronics and discuss their implications for spintronics. We then outline future avenues of research at the intersection of spintronics and orbitronics.
自旋电子学的终极目标之一是实现对自旋的高效电子操控,从而制造出高速、低功耗的纳米器件。实现这一目标的核心要素是电子轨道运动与自旋之间的相对论相互作用,但轨道角动量本身的特性在很大程度上仍未得到探索。然而,最近的理论和实验发现,在施加外部电场时,即使没有自旋轨道耦合,电子也可能获得非消失轨道角动量。这些发现推动了轨道电子学这一新兴领域的出现,该领域利用轨道角动量操纵磁性器件。在这篇综述中,我们将概述轨道电子学的最新发展,并讨论它们对自旋电子学的影响。然后,我们将概述自旋电子学和轨道电子学交叉领域的未来研究方向。
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引用次数: 0
Slow and non-equilibrium dynamics due to electronic ferroelectricity in a strongly-correlated molecular conductor 强相关分子导体中电子铁电引起的慢速非平衡动力学
Pub Date : 2024-06-28 DOI: 10.1038/s44306-024-00022-7
Tatjana Thomas, Yassine Agarmani, Steffi Hartmann, Mark Kartsovnik, Natalia Kushch, Stephen M. Winter, Sebastian Schmid, Peter Lunkenheimer, Michael Lang, Jens Müller
Ferroelectricity, where electronic degrees of freedom determine the polar order—thereby enabling fast switching and phase control—is an important research field in current condensed-matter physics. Using a combination of resistance noise and dielectric spectroscopy we investigate the nature of relaxor-type electronic ferroelectricity in the organic conductor κ-(BETS)2Mn[N(CN)2]3, a system that represents a wider class of materials of correlated electron systems for which functionalities for organic spintronics recently have been discussed. The two complementary spectroscopies reveal a distinct low-frequency dynamics on different length scales, namely (i) an intrinsic relaxation that is typical for relaxor ferroelectrics which classifies the system as a possible new multiferroic, and (ii) two-level processes which we identify as fluctuating polar nanoregions (PNR), i.e., clusters of quantum electric dipoles that fluctuate collectively. The PNR preform above the metal insulator (MI) transition. Upon cooling through TMI, a drastic increase of the low-frequency 1/f-type fluctuations and slowing down of the charge carrier dynamics is accompanied by the onset of strong non-equilibrium dynamics indicating a glassy transition of interacting dipolar clusters. The freezing of PNR and non-equilibrium dynamics is suggested to be a common feature of organic relaxor-type electronic ferroelectrics.
铁电性是当前凝聚态物理学的一个重要研究领域,在铁电性中,电子自由度决定极序,从而实现快速开关和相位控制。我们结合电阻噪声和介电光谱,研究了有机导体κ-(BETS)2Mn[N(CN)2]3 中弛豫型电子铁电的性质。两种互补光谱揭示了不同长度尺度上的独特低频动力学,即(i)弛豫铁电典型的本征弛豫,它将该系统归类为一种可能的新型多铁电体,以及(ii)两级过程,我们将其确定为波动极性纳米区域(PNR),即集体波动的量子电偶极子簇。PNR 预形成于金属绝缘体(MI)转变之上。冷却至 TMI 时,低频 1/f 型波动急剧增加,电荷载流子动力学放缓,同时出现了强烈的非平衡动力学,表明相互作用的偶极簇发生了玻璃化转变。PNR 和非平衡动力学的冻结被认为是有机弛豫型电子铁电的一个共同特征。
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引用次数: 0
Formation of chirality in propagating spin waves 传播自旋波中手性的形成
Pub Date : 2024-06-28 DOI: 10.1038/s44306-024-00026-3
Cody Trevillian, Vasyl Tyberkevych
A general approach to quantify chirality, or absence of parity symmetry, of spin waves has been developed and applied to spin waves propagating in obliquely magnetized ferromagnetic films. Using theoretical arguments and numerical calculations, it is shown that, upon increasing spin wave wavevector, initially achiral spin waves develop chiral properties through the “parity exchange” mechanism, which implies, in particular, that chiral spin waves appear in pairs. The most striking example of the parity exchange mechanism is the simultaneous formation of two chiral waves: the magnetostatic surface wave and the recently discovered heterosymmetric spin wave, which were previously considered independent of each other. Another manifestation of the parity exchange is the formation of strongly chiral waves near the anti-crossings of spin wave branches of unequal symmetry. These findings illustrate viable paths to engineering spin wave systems with prescribed chiral spectra that had not previously been considered.
我们开发了一种量化自旋波手性或缺乏奇偶对称性的通用方法,并将其应用于在斜磁化铁磁薄膜中传播的自旋波。理论论证和数值计算表明,随着自旋波波矢量的增加,最初的非手性自旋波通过 "奇偶性交换 "机制发展出手性特性,这尤其意味着手性自旋波成对出现。奇偶性交换机制最显著的例子是同时形成两种手性波:磁静表面波和最近发现的异对称自旋波,而这两种波之前被认为是相互独立的。奇偶性交换的另一种表现形式是在不对称自旋波分支的反交叉点附近形成强手性波。这些发现说明了设计具有规定手性谱的自旋波系统的可行途径,而这是以前从未考虑过的。
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引用次数: 0
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